Quantum cryptography

Quantum cryptography is the science of exploiting quantum mechanical properties to perform cryptographic tasks. The best known example of quantum cryptography is quantum key distribution which offers an information-theoretically secure solution to the key exchange problem. Currently used popular public-key encryption and signature schemes (e.g., RSA and ElGamal) can be broken by quantum adversaries. The advantage of quantum cryptography lies in the fact that it allows the completion of various cryptographic tasks that are proven or conjectured to be impossible using only classical (i.e. non-quantum) communication (see below for examples). For example, it is impossible to copy data encoded in a quantum state and the very act of reading data encoded in a quantum state changes the state. This is used to detect eavesdropping in quantum key distribution.

History

Quantum cryptography was proposed first by Stephen Wiesner, then at Columbia University in New York, who, in the early 1970s, introduced the concept of quantum conjugate coding. His seminal paper titled "Conjugate Coding" was rejected by IEEE Information Theory Society, but was eventually published in 1983 in SIGACT News (15:1 pp. 78–88, 1983). In this paper he showed how to store or transmit two messages by encoding them in two "conjugate observables", such as linear and circular polarization of light, so that either, but not both, of which may be received and decoded. He illustrated his idea with a design of unforgeable bank notes. In 1984, building upon this work, Charles H. Bennett, of the IBM's Thomas J. Watson Research Center, and Gilles Brassard, of the Université de Montréal, proposed a method for secure communication based on Wiesner’s "conjugate observables", which is now called BB84.[1] In 1991 Artur Ekert developed a different approach to quantum key distribution based on peculiar quantum correlations known as quantum entanglement.[2]

Random rotations of the polarization by both parties (usually called Alice and Bob) have been proposed in Kak's three-stage quantum cryptography protocol.[3] In principle, this method can be used for continuous, unbreakable encryption of data if single photons are used.[4] The basic polarization rotation scheme has been implemented.[5]

The BB84 method is at the basis of quantum key distribution methods. Companies that manufacture quantum cryptography systems include MagiQ Technologies, Inc. of Boston, ID Quantique of Geneva, Switzerland, QuintessenceLabs (Canberra, Australia) and SeQureNet (Paris).

Quantum key distribution

The most well known and developed application of quantum cryptography is quantum key distribution (QKD), which is the process of using quantum communication to establish a shared key between two parties (Alice and Bob, for example) without a third party (Eve) learning anything about that key, even if Eve can eavesdrop on all communication between Alice and Bob. This is achieved by Alice encoding the bits of the key as quantum data and sending them to Bob; if Eve tries to learn these bits, the messages will be disturbed and Alice and Bob will notice. The key is then typically used for encrypted communication using classical techniques. For instance, the exchanged key could be used as the seed of the same random number generator both by Alice and Bob.

The security of QKD can be proven mathematically without imposing any restrictions on the abilities of an eavesdropper, something not possible with classical key distribution. This is usually described as "unconditional security", although there are some minimal assumptions required including that the laws of quantum mechanics apply and that Alice and Bob are able to authenticate each other, i.e. Eve should not be able to impersonate Alice or Bob as otherwise a man-in-the-middle attack would be possible.

One aspect of QKD is that it is secure against quantum computers, as its strength does not depend on mathematical complexity, like post-quantum cryptography, but on physical principles.

Quantum commitment

Following the discovery of quantum key distribution and its unconditional security, researchers tried to achieve other cryptographic tasks with unconditional security. One such task was commitment. A commitment scheme allows a party Alice to fix a certain value (to "commit") in such a way that Alice cannot change that value while at the same time ensuring that the recipient Bob cannot learn anything about that value until Alice decides to reveal it. Such commitment schemes are commonly used in cryptographic protocols. In the quantum setting, they would be particularly useful: Crépeau and Kilian showed that from a commitment and a quantum channel, one can construct an unconditionally secure protocol for performing so-called oblivious transfer.[6] Oblivious transfer, on the other hand, had been shown by Kilian to allow implementation of almost any distributed computation in a secure way (so-called secure multi-party computation).[7] (Notice that here we are a bit imprecise: The results by Crépeau and Kilian[6] and Kilian[7] together do not directly imply that given a commitment and a quantum channel one can perform secure multi-party computation. This is because the results do not guarantee "composability", that is, when plugging them together, one might lose security. Later works showed, however, how composability can be ensured in this setting.)

Unfortunately, early quantum commitment protocols[8] were shown to be flawed. In fact, Mayers showed that (unconditionally secure) quantum commitment is impossible: a computationally unlimited attacker can break any quantum commitment protocol.[9]

Yet, the result by Mayers does not preclude the possibility of constructing quantum commitment protocols (and thus secure multi-party computation protocols) under assumptions that they are much weaker than the assumptions needed for commitment protocols that do not use quantum communication. The bounded quantum storage model described below is an example for a setting in which quantum communication can be used to construct commitment protocols. A breakthrough in November 2013 offers “unconditional” security of information by harnessing quantum theory and relativity, which has been successfully demonstrated on a global scale for the first time.[10]

Bounded- and noisy-quantum-storage model

One possibility to construct unconditionally secure quantum commitment and quantum oblivious transfer (OT) protocols is to use the bounded quantum storage model (BQSM). In this model, we assume that the amount of quantum data that an adversary can store is limited by some known constant Q. We do not, however, impose any limit on the amount of classical (i.e., non-quantum) data the adversary may store.

In the BQSM, one can construct commitment and oblivious transfer protocols.[11] The underlying idea is the following: The protocol parties exchange more than Q quantum bits (qubits). Since even a dishonest party cannot store all that information (the quantum memory of the adversary is limited to Q qubits), a large part of the data will have to be either measured or discarded. Forcing dishonest parties to measure a large part of the data allows to circumvent the impossibility result by Mayers;[9] commitment and oblivious transfer protocols can now be implemented.

The protocols in the BQSM presented by Damgård, Fehr, Salvail, and Schaffner[11] do not assume that honest protocol participants store any quantum information; the technical requirements are similar to those in QKD protocols. These protocols can thus, at least in principle, be realized with today's technology. The communication complexity is only a constant factor larger than the bound Q on the adversary's quantum memory.

The advantage of the BQSM is that the assumption that the adversary's quantum memory is limited is quite realistic. With today's technology, storing even a single qubit reliably over a sufficiently long time is difficult. (What "sufficiently long" means depends on the protocol details. By introducing an artificial pause in the protocol, the amount of time over which the adversary needs to store quantum data can be made arbitrarily large.)

An extension of the BQSM is the noisy-storage model introduced by Wehner, Schaffner and Terhal.[12] Instead of considering an upper bound on the physical size of the adversary's quantum memory, an adversary is allowed to use imperfect quantum storage devices of arbitrary size. The level of imperfection is modelled by noisy quantum channels. For high enough noise levels, the same primitives as in the BQSM can be achieved [13] and the BQSM forms a special case of the noisy-storage model.

In the classical setting, similar results can be achieved when assuming a bound on the amount of classical (non-quantum) data that the adversary can store.[14] It was proven, however, that in this model also the honest parties have to use a large amount of memory (namely the square-root of the adversary's memory bound).[15] This makes these protocols impractical for realistic memory bounds. (Note that with today's technology such as hard disks, an adversary can cheaply store large amounts of classical data.)

Position-based quantum cryptography

The goal of position-based quantum cryptography is to use the geographical location of a player as its (only) credential. For example, one wants to send a message to a player at a specified position with the guarantee that it can only be read if the receiving party is located at that particular position. In the basic task of position-verification, a player Alice wants to convince the (honest) verifiers that she is located at a particular point. It has been shown by Chandran et al. that position-verification using classical protocols is impossible against colluding adversaries (who control all positions except the prover's claimed position).[16] Under various restrictions on the adversaries, schemes are possible.

Under the name of 'quantum tagging', the first position-based quantum schemes have been investigated in 2002 by Kent. A US-patent[17] was granted in 2006, but the results only appeared in the scientific literature in 2010.[18] After several other quantum protocols for position verification have been suggested in 2010,[19][20] Buhrman et al. were able to show a general impossibility result:[21] using an enormous amount of quantum entanglement (they use a doubly exponential number of EPR pairs, in the number of qubits the honest player operates on ), colluding adversaries are always able to make it look to the verifiers as if they were at the claimed position. However, this result does not exclude the possibility of practical schemes in the bounded- or noisy-quantum-storage model (see above). Later Beigi and König improved the amount of EPR pairs needed in the general attack against position-verification protocols to exponential. They also showed that a particular protocol remains secure against adversaries who controls only a linear amount of EPR pairs.[22]

Device-independent quantum cryptography

A quantum cryptographic protocol is device-independent if its security does not rely on trusting that the quantum devices used are truthful. Thus the security analysis of such a protocol needs to consider scenarios of imperfect or even malicious devices. Mayers and Yao[23] proposed the idea of designing quantum protocols using "self-testing" quantum apparatus, the internal operations of which can be uniquely determined by their input-output statistics. Subsequently, Roger Colbeck in his Thesis[24] proposed the use of Bell tests for checking the honesty of the devices. Since then, several problems have been shown to admit unconditional secure and device-independent protocols, even when the actual devices performing the Bell test are substantially "noisy," i.e., far from being ideal. These problems include quantum key distribution,[25][26] randomness expansion,[26][27] and randomness amplification.[28]

Post-quantum cryptography

Quantum computers may become a technological reality; it is therefore important to study cryptographic schemes used against adversaries with access to a quantum computer. The study of such schemes is often referred to as post-quantum cryptography. The need for post-quantum cryptography arises from the fact that many popular encryption and signature schemes (such as RSA and its variants, and schemes based on elliptic curves) can be broken using Shor's algorithm for factoring and computing discrete logarithms on a quantum computer. Examples for schemes that are, as of today's knowledge, secure against quantum adversaries are McEliece and lattice-based schemes. Surveys of post-quantum cryptography are available.[29][30]

There is also research into how existing cryptographic techniques have to be modified to be able to cope with quantum adversaries. For example, when trying to develop zero-knowledge proof systems that are secure against quantum adversaries, new techniques need to be used: In a classical setting, the analysis of a zero-knowledge proof system usually involves "rewinding", a technique that makes it necessary to copy the internal state of the adversary. In a quantum setting, copying a state is not always possible (no-cloning theorem); a variant of the rewinding technique has to be used.[31]

Post quantum algorithms are also called “quantum resistant”, because – unlike QKD – it is not known or provable that there will not be potential future quantum attacks against them. Even though they are not vulnerable to Shor’s algorithm the NSA are announcing plans to transition to quantum resistant algorithms.[32]

References

  1. ↑ Bennett, C.H. and G. Brassard. Quantum cryptography: Public key distribution and coin tossing. In Proceedings of IEEE International Conference on Computers, Systems and Signal Processing, volume 175, page 8. New York, 1984.
  2. ↑ Ekert. A. Physical Review Letters, 67, pp.661-663, (1991)
  3. ↑ Kak, S., A three-stage quantum cryptography protocol. Foundations of Physics Letters, vol. 19, pp.293-296, 2006.
  4. ↑ Chen, Y. et al., Embedded security framework for integrated classical and quantum cryptography in optical burst switching networks. Security and Communication Networks, vol. 2, pp. 546-554, 2009.
  5. ↑ http://www.kurzweilai.net/a-multi-photon-approach-to-quantum-cryptography
  6. 1 2 Crépeau, Claude; Joe, Kilian (1988). Achieving Oblivious Transfer Using Weakened Security Assumptions (Extended Abstract). FOCS 1988. IEEE. pp. 42–52.
  7. 1 2 Kilian, Joe (1988). Founding cryptography on oblivious transfer. STOC 1988. ACM. pp. 20–31.
  8. ↑ Brassard, Gilles; Claude, Crépeau; Jozsa, Richard; Langlois, Denis (1993). A Quantum Bit Commitment Scheme Provably Unbreakable by both Parties. FOCS 1993. IEEE. pp. 362–371.
  9. 1 2 Mayers, Dominic (1997). "Unconditionally Secure Quantum Bit Commitment is Impossible". Physical Review Letters (APS) 78 (17): 3414–3417. arXiv:quant-ph/9605044. Bibcode:1997PhRvL..78.3414M. doi:10.1103/PhysRevLett.78.3414. Preprint at arXiv:quant-ph/9605044v2
  10. ↑ "Experimental Bit Commitment Based on Quantum Communication and Special Relativity".
  11. 1 2 Damgård, Ivan; Fehr, Serge; Salvail, Louis; Schaffner, Christian (2005). Cryptography In the Bounded Quantum-Storage Model. FOCS 2005. IEEE. pp. 449–458. A full version is available at arXiv:quant-ph/0508222.
  12. ↑ Wehner, Stephanie; Schaffner, Christian; Terhal, Barbara M. (2008). "Cryptography from Noisy Storage". Physical Review Letters (APS) 100 (22): 220502. arXiv:0711.2895. Bibcode:2008PhRvL.100v0502W. doi:10.1103/PhysRevLett.100.220502. PMID 18643410. A full version is available at arXiv:0711.2895.
  13. ↑ Koenig, Robert; Wehner, Stephanie; Wullschleger, Juerg. "Unconditional security from noisy quantum storage". A full version is available at arXiv:0906.1030.
  14. ↑ Cachin, Christian; Crépeau, Claude; Marcil, Julien (1998). Oblivious Transfer with a Memory-Bounded Receiver. FOCS 1998. IEEE. pp. 493–502.
  15. ↑ Dziembowski, Stefan; Ueli, Maurer (2004). On Generating the Initial Key in the Bounded-Storage Model. Eurocrypt 2004. LNCS. Springer. pp. 126–137. Preprint available at .
  16. ↑ Chandran, Nishanth; Moriarty, Ryan; Goyal, Vipul; Ostrovsky, Rafail (2009). Position-Based Cryptography. A full version is available at IACR eprint:2009/364.
  17. ↑ US 7075438, issued 2006-07-11
  18. ↑ Kent, Adrian; Munro, Bill; Spiller, Tim (2010). "Quantum Tagging with Cryptographically Secure Tags". A full version is available at arXiv:1008.2147.
  19. ↑ Lau, Hoi-Kwan; Lo, Hoi-Kwong (2010). "Insecurity of position-based quantum-cryptography protocols against entanglement attacks". Physical Review A (APS) 83: 012322. arXiv:1009.2256. Bibcode:2011PhRvA..83a2322L. doi:10.1103/PhysRevA.83.012322. A full version is available at arXiv:1009.2256.
  20. ↑ Malaney, Robert A. (2010). "Location-dependent communications using quantum entanglement". Physical Review A 81: 042319. arXiv:1003.0949. Bibcode:2010PhRvA..81d2319M. doi:10.1103/PhysRevA.81.042319.
  21. ↑ Buhrman, Harry; Chandran, Nishanth; Fehr, Serge; Gelles, Ran; Goyal, Vipul; Ostrovsky, Rafail; Schaffner, Christian (2010). "Position-Based Quantum Cryptography: Impossibility and Constructions". A full version is available at arXiv:1009.2490.
  22. ↑ Beigi, Salman; König, Robert (2011). "Simplified instantaneous non-local quantum computation with applications to position-based cryptography". arXiv:1101.1065.
  23. ↑ Mayers, Dominic; Yao, Andrew C.-C. (1998). Quantum Cryptography with Imperfect Apparatus. IEEE Symposium on Foundations of Computer Science (FOCS). arXiv:quant-ph/9809039. horizontal tab character in |conference= at position 43 (help)
  24. ↑ Colbeck, Roger (December 2006). "Chapter 5". Quantum And Relativistic Protocols For Secure Multi-Party Computation (Thesis). University of Cambridge.
  25. ↑ Vazirani, Umesh; Vidick, Thomas (2014). "Fully Device-Independent Quantum Key Distribution". Physical Review Letters 113: 140501. arXiv:1403.3830. Bibcode:2014PhRvL.113b0501A. doi:10.1103/PhysRevLett.113.020501.
  26. 1 2 Miller, Carl; Shi, Yaoyun (2014). "Robust protocols for securely expanding randomness and distributing keys using untrusted quantum devices". arXiv:1402.0489.
  27. ↑ Miller, Carl; Shi, Yaoyun (2015). "Universal security for randomness expansion". arXiv:1411.6608.
  28. ↑ Chung, Kai-Min; Shi, Yaoyun; Wu, Xiaodi (2014). "Physical Randomness Extractors: Generating Random Numbers with Minimal Assumptions". arXiv:1402.4797.
  29. ↑ "Post-quantum cryptography". Retrieved 29 August 2010.
  30. ↑ Bernstein, Daniel J.; Buchmann, Johannes; Dahmen, Erik, eds. (2009). Post-quantum cryptography. Springer. ISBN 978-3-540-88701-0.
  31. ↑ Watrous, John (2009). "Zero-Knowledge against Quantum Attacks". SIAM J. Comput. 39 (1): 25–58. doi:10.1137/060670997.
  32. ↑ "NSA Suite B Cryptography". Retrieved 29 December 2015.
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